The Chiral Magnetic Effect and anomaly-induced transport

被引：416

作者：

Kharzeev, Dmitri E. ^{[1
,2
]}

机构：

[1] SUNY Stony Brook, Dept Phys & Astron, Stony Brook, NY 11794 USA

[2] Brookhaven Natl Lab, Dept Phys, Upton, NY 11973 USA

来源：

PROGRESS IN PARTICLE AND NUCLEAR PHYSICS | 2014年 / 75卷

关键词：

Chiral anomaly; Chiral magnetic effect; HEAVY-ION COLLISIONS; QUARK-GLUON PLASMA; PARITY VIOLATION; FIELD-THEORY; QCD; EQUILIBRIUM; FLUCTUATIONS; POLARIZATION; TEMPERATURE; MOMENTUM;

D O I：

10.1016/j.ppnp.2014.01.002

中图分类号：

O57 [原子核物理学、高能物理学];

学科分类号：

070202 ;

摘要：

The Chiral Magnetic Effect (CME) is the phenomenon of electric charge separation along the external magnetic field that is induced by the chirality imbalance. The CME is a macroscopic quantum effect - it is a manifestation of the chiral anomaly creating a collective motion in Dirac sea. Because the chirality imbalance is related to the global topology of gauge fields, the CME current is topologically protected and hence non-dissipative even in the presence of strong interactions. As a result, the CME and related quantum phenomena affect the hydrodynamical and transport behavior of systems possessing chiral fermions, from the quark-gluon plasma to chiral materials. The goal of the present review is to provide an elementary introduction into the main ideas underlying the physics of CME, a historical perspective, and a guide to the rapidly growing literature on this topic. (C) 2014 Elsevier B.V. All rights reserved.

引用

页码：133 / 151

页数：19

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